Propionic Acid Outperforms Formic and Acetic Acid in MS Sensitivity for High-Flow Reversed-Phase LC-MS Bottom-Up Proteomics

<p><strong>This study introduces a quantitative workflow for multielement single-cell analysis by mass cytometry using metal-loaded, multielement-barcoded polystyrene beads as calibration standards. Online mixing allows bead and cell events to be distinguished by TOF-MS, enabling elemental concentrations in labeled cells to be quantified from bead responses.</strong></p><p>The approach was demonstrated with Lu-, Nd-, and Ir-labeled cancer cells and extended through a polynomial calibration model to elements not directly included in the beads. Agreement with external calibration highlights the method’s potential as a universal quantitative strategy for mass cytometry and single-cell ICP-TOF-MS.</p><blockquote><h4><strong>The original article</strong></h4><h4><a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/ancham/article/98/31/22966/5231419/Quantitative-Single-Cell-Multielemental-Analysis#249383980"><strong>Quantitative Single-Cell Multielemental Analysis Using Metal-Loaded Microparticles: toward a Universal Quantification Workflow in Mass Cytometry</strong></a></h4><p>Ángela de la Rosa-Díaz; Carlos López-Portugués; Mario Corte-Rodríguez*; María Montes-Bayón *</p><p>Anal. Chem. (2026) 98 (31): 22966–22976</p><div><a target="_blank" rel="noopener noreferrer" href="https://doi.org/10.1021/acs.analchem.6c02340">https://doi.org/10.1021/acs.analchem.6c02340</a></div><h6>licensed under <a target="_blank" rel="noopener noreferrer" href="https://creativecommons.org/licenses/by/4.0/"><strong>CC-BY 4.0</strong></a></h6></blockquote><p><strong>Selected sections from the article follow. Formats and hyperlinks were adapted from the original.</strong></p><div><div><div><div><div><p>Understanding the biochemical and functional heterogeneity of individual cells is a central challenge in modern biology, immunology, oncology, and clinical translational research. Flow cytometry, and, more recently, spectral flow cytometry, (<a href="javascript:;">1</a>) have become essential tools for high-dimensional single-cell analysis. However, obtaining robust quantitative information at the single-cell level remains challenging, particularly when comparing measurements across experiments and laboratories. Quantitative approaches have been developed for fluorescence flow cytometry, typically relying on calibration beads and standardized antibody conjugates to improve interexperimental comparability. (<a href="javascript:;">2−4</a>) Nevertheless, the accuracy of these methods remains influenced by fluorophore-specific properties and labeling variability, highlighting the need for alternative quantitative single-cell analytical strategies.</p></div><div><p>Mass cytometry, or cytometry by time-of-flight (CyTOF), which was introduced by the team of Bandura in 2009, has emerged as a technological breakthrough by substituting fluorophores with isotopically pure metal tags, whose signals are detected by TOF elemental mass spectrometry (MS) using an inductively coupled plasma as ion source (ICP–TOF–MS). (<a href="javascript:;">5</a>) This technology has allowed to remove nearly all spectral overlaps and enabled experiments that can routinely include 40–60 parameters, including not only protein biomarkers but also DNA markers and metallodrugs or nanoparticles. (<a href="javascript:;">6, 7</a>) Numerous studies have taken advantage of the highly multiplex capabilities of CyTOF to investigate immune responses, characterize tumor-infiltrating lymphocytes, or follow hematopoietic differentiation with greater resolution than was previously possible. (<a href="javascript:;">8−10</a>) Indeed, the technique has become central to many multiparametric immunology pipelines by facilitating deeper functional analyses, from mapping subtle cell-cycle states (<a href="javascript:;">11</a>) to profiling intracellular cytokine signatures and activation markers (<a href="javascript:;">12</a>) that are often difficult to resolve by fluorescence-based approaches. (<a href="javascript:;">13</a>)</p></div><div><p>Beyond its multiplexing capability, an often overlooked advantage of mass cytometry is its potential for elemental quantification. Unlike fluorescence-based approaches, ICP–MS-based detection enables direct conversion of signal intensities into elemental amounts through established calibration strategies. This principle, successfully applied for single-cell elemental analysis by ICP–MS (SC–ICP–MS), has shown to be suitable in different applications. Thus, quantification of intrinsic (<a href="javascript:;">14−17</a>) or exogenous (<a href="javascript:;">18−20</a>) elements, as well as protein biomarkers following metal-labeling strategies (<a href="javascript:;">21, 22</a>) compare well with the bulk analyses on the same cell suspension. However, despite the efforts made to develop quantitative strategies, mass cytometry remains as a mainly qualitative strategy, where very few approaches have explored its unquestionable quantification potential. (<a href="javascript:;">4, 23−25</a>)</p></div><div><p>CyTOF data quality depends critically on managing instrumental variability. Plasma fluctuations, partial clogging of the sample introduction system or injector and periodic retuning, introduce changes in sensitivity that can obscure biological differences between samples measured at different times or in different instruments. To mitigate these effects, CyTOF applies multielement calibration polymeric beads, such as EQ six-element calibration beads, that are mixed with every sample at a fixed concentration before nebulization. (<a href="javascript:;">26, 27</a>) These beads, containing defined quantities of yttrium, indium, cerium, terbium, lutetium and bismuth, allow computational normalization and provide a reference signal that corrects for shifts in sensitivity over time. More recently, approaches using frozen antibody master mixes, unified acquisition templates, and sophisticated normalization algorithms have been introduced to enable reproducible multibatch studies and harmonize data sets across different research centers. (<a href="javascript:;">27, 28</a>)</p></div><div><p>Since the sought beads that contain multiple elements in a wide mass range (from <sup>89</sup>Y to <sup>209</sup>Bi) are commercially available and show high reproducibility, they could serve as quantitative (single-point) analytical standards (once characterized accordingly). This use would increase their analytical value not only as mere drift correctors but also as calibrants that are present within the sample (matrix-matched). Such a strategy is aligned with recently proposed particle-based calibration approaches in SP/SC–ICP–MS, which exploit transient events of the same nature as the analyte to avoid transport-efficiency-related uncertainties. (<a href="javascript:;">29</a>) In this way, the estimation of parameters like transport efficiencies of the ionic standards is eliminated, reducing the associated uncertainties. Moreover, since the beads are routinely added to all samples in CyTOF, any raw data file could be reprocessed at any time to extract any quantitative information without any additional measurements.</p></div><div><p>Despite their routine use for signal normalization, CyTOF calibration beads have not been systematically explored as quantitative standards for single-cell elemental analyses. Their use for quantification implies several analytical challenges, including the accurate characterization of their elemental content, the translation of bead-derived responses into cellular elemental amounts, and the extension of the calibration strategy to isotopes that are not present in the beads. Addressing these challenges is essential before calibration beads can be used as reliable quantitative reference.</p></div><div><p>An interesting additional feature of plasma-based techniques is their relatively uniform sensitivity across the entire mass range. It has been described that the observed instrumental response in most ICP–MS can be fitted to a simple equation as a function of the <i>m</i>/<i>z</i> of the isotope to be measured for the elements with similar ionization in the plasma, such as the lanthanides. (<a href="javascript:;">30, 31</a>) If the transient signals of the multielemental beads are used to obtain the instrumental responses and these are empirically modeled across the monitored <i>m</i>/<i>z</i> range, a practical route toward multielemental quantification strategy is obtained. This would represent a quantification workflow for multiplex single-cell elemental analysis that repurposes multielement CyTOF calibration beads as generic standards. Such an approach seeks to address the limitations in calibration procedures and, ultimately, to enhance the quantitative applications of high-dimensional single-cell MS that can be applied not only to CyTOF-based analysis but could also be extended to any other SC–ICP–MS analysis using any other TOF mass analyzers.</p><h4><strong>Experimental Section</strong></h4><h5><strong>Instrumentation</strong></h5><div><p>The single-particle ICP–MS measurements were performed by using the <a target="_blank" rel="noopener noreferrer" href="https://labrulez.com/en-us/all/products/1206"><strong>iCAP TQ triple quadrupole ICP–MS system</strong></a> from Thermo Fisher Scientific (Bremen, Germany). All measurements were done using the standard configuration for sample introduction, including the Micro-Mist nebulizer at a sample flow rate of 0.4 mL min<sup>–1</sup> and a cyclonic spray chamber. The sample introduction setup was used together with a T<strong>eledyne Cetac ASX-560 autosampler.</strong> SP-ICP-MS characterizacion of the lanthanide-loaded polystyrene beads was carried out setting a dwell time of 5 ms. Daily optimization of ICP–MS was performed to enhance signal sensitivity, ensuring that the generation of oxide ions and doubly charged species remained below 3% and 5%, respectively.</p></div><div><p>The CyTOF experiments were conducted in a <strong>CyTOF XT</strong> (Standard BioTools, San Francisco, CA, USA). This instrument is an ICP–MS that operates TOF mass analyzer with a shortened mass coverage from <i>m</i>/<i>z</i> 75 to 209. The samples are placed in a refrigerated carousel at 4 <span>°</span>C and injected into the CyTOF with a hydraulic autosampler that is able to handle sample introduction and system washing. The autosampler automatically adds the EQ6 calibration beads (Standard BioTools) to every sample at a 1:10 dilution. After mixing, the bead-containing sample is injected at 30 μL·min<sup>–1</sup> through a pneumatic nebulizer and a spray chamber that is heated at 200 <span>°</span>C. using a constant sample flow of at 10 μL min<sup>–1</sup>. Microparticle imaging was carried out with a <strong>JEOL JEM-2100F transmission electron microscope.</strong></p><h4><strong>Results and Discussion</strong></h4><h5><strong>BiRM: An Interpolated Model for Multielement Quantification</strong></h5><p>Taking advantage of the multielemental composition of the beads uniformly distributed along the CyTOF measuring range, their molar response factors can be estimated and plotted against the <i>m</i>/<i>z</i> of each of the isotopes contained on the beads. This is possible thanks to the high ionization efficiency achievable in the plasma for the elements of the beads that is close to 100%. In that case, previous publications demonstrated that the ICP–MS molar response can be modeled using different theoretical equations. (<a href="javascript:;">30, 31</a>) Consequently, the molar responses (<i>n</i><sub>resp</sub>) for all the 8 isotopes of the 6 elements contained in the beads (typically &gt;5000 events) were calculated as in <a href="javascript:;">eq 3</a> and represented against the mass-to-charge ratio (<i>m</i>/<i>z</i>). The molar response, differently to the previously reported response factor (α<sub>i</sub>), takes into account the atomic mass of the element and isotope, the isotope abundance, and the concentration. This response was fitted empirically to polynomial functions of degree 2, 3, 4, and 5, resulting in the quartic function the one with the best correlation (<i>r</i><sup>2</sup> = 0.99) while avoiding overfitting of the data. The response factors for all the isotopes are represented in <a href="javascript:;">Figure 4</a> (every data point considered for the fitting corresponds to the average intensity obtained for a minimum of 5000 bead events and the corresponding standard deviation), together with the fitted quartic polynomial function of <a href="javascript:;">eq 4</a>. This behavior showing a mass-dependent response with a slight decrease at high <i>m</i>/<i>z</i> is also consistent with published results using ICP–TOF–MS instruments. (<a href="javascript:;">34</a>) The fourth-order polynomial was used as an empirical interpolation of the instrumental response within the calibrated mass range in our specific CyTOF instrument, without physical significance of the coefficients.</p><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Anal_Chem_2026_98_31_22966_22976_Figure_4_Molar_response_factors_for_every_isotope_in_the_beads_b8317c3de7.jpg" alt="Anal. Chem. (2026) 98 (31): 22966–22976: Figure 4. Molar response factors for every isotope in the beads as a function of m/z and the quartic function model (dashed line) that fits such data obtained using CyTOF results. Standard deviation of each data point is also included (only distinguishable in the case of 140Ce)." srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Anal_Chem_2026_98_31_22966_22976_Figure_4_Molar_response_factors_for_every_isotope_in_the_beads_b8317c3de7.jpg 245w," sizes="100vw" width="996" height="492"></p><p>Using the <i>m</i>/<i>z</i> of the isotope of interest and by interpolation in the curve, it is possible to estimate its molar response on each sample (matrix matched). Out of the obtained molar response and taking the integrated dual counts obtained for such isotope in the sample, inferring its mass in a single cell event is straightforward. <a href="javascript:;">Figure 5</a>A shows the correlation between the predicted (using <a href="javascript:;">eq 4</a>) and the experimental value (using <a href="javascript:;">eq 3</a>) for the molar responses of the isotopes contained in the beads. A good correlation can be observed (<i>R</i><sup>2</sup> = 0.99), with a slope of 0.99, suggesting an excellent ability of the model to calculate the molar sensitivity of these isotopes.</p><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Anal_Chem_2026_98_31_22966_22976_Figure_5_A_Plot_showing_the_correlation_between_the_Bi_RM_predicted_and_the_experimental_molar_response_for_the_multielemental_beads_6acfc9378b.jpg" alt="Anal. Chem. (2026) 98 (31): 22966–22976: Figure 5. (A) Plot showing the correlation between the BiRM-predicted and the experimental molar response for the multielemental beads and (B) the correlation of 8200 individual cell events obtained by BiRM versus calibration with 175Lu standards. Error bars were omitted for clarity. Experimental uncertainties associated with the molar response factors are reported in Table 2." srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Anal_Chem_2026_98_31_22966_22976_Figure_5_A_Plot_showing_the_correlation_between_the_Bi_RM_predicted_and_the_experimental_molar_response_for_the_multielemental_beads_6acfc9378b.jpg 116w," sizes="100vw" width="997" height="1336"></p><p>Although it is possible to perform the described calculations using a datasheet like from microsoft excel, Google Sheets, or LibreOffice Calc, the BiRM interpolation and quantification workflow becomes increasingly cumbersome as the number of isotopes, events and biological replicates grows. For this reason, an in-house script has been developed in R, which is provided as <a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/ancham/article-supplement/5231419/pdf/ac6c02340_si_001/">Supporting Information</a>. The script, which is fully transparent and open-access, operates directly on the data matrix generated for either cell events or calibration-bead events after standard CyTOF preprocessing (see the Experimental section). By introducing the elemental information required for BiRM calculations as described in the accompanying “Readme” file, the script automatically computes the molar or mass amount of each element per cell. In addition, it generates summary statistics, diagnostic figures and histograms for rapid quality assessment. This implementation ensures reproducibility, minimizes operator-dependent variability and allows users to reprocess previously acquired data sets without any additional experimental steps. A continuously updated version of software will be made available in a public repository, where future improvements, extension and documentation will be deposited. Because the isotopes used in <a href="javascript:;">Figure 5</a>A were also employed to construct the BiRM model, an additional leave-one-out validation was performed to assess its predictive capability. In each iteration, one calibration isotope was excluded from the fitting procedure and its molar response factor was subsequently predicted using a model constructed from the remaining isotopes. The predicted values were then compared with the experimentally determined molar response factors. The leave-one-out validation yielded a mean absolute relative error (MARE) of 14.3%, compared with 8.3% for the all-in model. As expected, prediction errors increased when an isotope was excluded from the model construction. However, the obtained deviations remained within a reasonable range considering the limited number of calibration points available for model fitting.</p><h4><strong>Conclusion</strong></h4><p>This study presents a practical route to quantitative mass cytometry by repurposing the multielement calibration beads that are routinely added to CyTOF samples as in-tube quantitative standards that can be extended not only to CyTOF but also to any other TOF-based ICP–MS instruments. Two complementary strategies were proposed. First, BaQS performs single-point calibration for bead-encoded isotopes to obtain the absolute mass of lanthanide per cell. Second, the BiRM makes use of the multielement bead signature to empirically model the instrumental response across the monitored <i>m</i>/<i>z</i> window, enabling the prediction of response factors for isotopes that are not present in the beads. The results indicate that both strategies provided accurate results with no statistically significant differences with the validated external standards calibration for the quantification of bead-contained and noncontained lanthanides, being BaQS and BiRM simpler, faster, more efficient, and ready to be applied to already acquired data with no additional measurements needed.</p></div></div></div></div></div></div>

Quantitative Single-Cell Multielemental Analysis Using Metal-Loaded Microparticles: toward a Universal Quantification Workflow in Mass Cytometry

<p><strong>In the week from August 31, the following webinars await you in the field of atomic and molecular spectroscopy and spectrometry</strong></p><blockquote><h4><a target="_blank" rel="noopener noreferrer" href="https://icpms.labrulez.com/webinars"><strong>👉 DETAILS AND REGISTRATION IN THE WEBINARS SECTION</strong></a></h4><p><strong>👉 Search and filter in the largest global database</strong> with over <strong>5 500 GC, LC, MS and spectroscopy webinars</strong>.</p></blockquote><h5><strong>1. Technology Networks: Modern Methods for Faster Microbial Analysis</strong></h5><ul><li>Tu, 1.9.2026 11:00 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://labrulez.com/en-us/all/webinar/6454">Registration</a></li></ul><p>Struggling to choose the right technique for microbial testing? Learn how MALDI-TOF, FTIR, and automated DNA/RNA electrophoresis accelerate identification.</p><h5><strong>2. Agilent Technologies: ICP-MS for Hybrid Photoelectrode Characterization</strong></h5><ul><li>Tu, 1.9.2026 21:30 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://labrulez.com/en-us/all/webinar/6411">Registration</a></li></ul><p>Quantify catalyst loading on hybrid photoelectrodes and discover how the Agilent 7850 ICP-MS supports solar fuel research.</p><h5><strong>3. SciY/Mestrelab Research: From Legacy Workflows to Paperless Labs: Track Every Sample, Process, and Decision</strong></h5><ul><li>Th, 3.9.2026 17:00 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://labrulez.com/en-us/all/webinar/6425">Registration</a></li></ul><p>Transform your lab from paper to digital. Learn how WebLab and LIMS workflows automate sample tracking and support laboratory compliance.</p><h5><strong>4. Agilent Technologies: Learn to Select and Apply the Proper Internal Standard in ICP-OES</strong></h5><ul><li>Th, 3.9.2026 20:00 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://labrulez.com/en-us/all/webinar/6412">Registration</a></li></ul><p>Master the use of internal standards in ICP-OES and learn how to select suitable standards to correct matrix effects and signal drift.</p>

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LECO VX4 Compact Inverted Microscope

LECO VX4 is a compact inverted metallurgical microscope delivering high-resolution imaging, polarized light, and advanced optics for precise microstructural analysis in materials and educational labs.

<p><strong>The LECO VX Series metallurgical microscopes are advanced microscopy solutions designed for materials laboratories that require high-resolution imaging, reliable performance, and consistent metallographic results. Built with a strong focus on precision, repeatability, and ease of operation, the VX Series supports a wide range of applications across automotive, aerospace, academic research, and quality assurance laboratories.</strong></p><p>From routine microstructural evaluation to detailed failure investigations, the VX Series delivers the optical quality and robustness professionals expect. Integrated digital imaging systems and compatibility with LECO’s analytical software tools ensure efficient workflows, clear documentation, and scalable solutions for laboratories of all sizes. The <strong>VX3, VX4, and VX5 models</strong> allow laboratories to select the configuration that best matches their technical and budgetary requirements.</p><h4><strong>Why the VX Series Is Ideal for Metallography</strong></h4><p>LECO metallographic microscopes play a critical role in examining the microstructure of metals and alloys. This essential step in metallographic analysis enables detailed evaluation of grain size, phase distribution, and structural features, helping users identify defects and assess material quality. The high level of detail provided by the VX Series supports quality control, failure analysis, and materials inspection across a broad range of industries.</p><h4><strong>LECO VX4 Compact Inverted Microscope</strong></h4><p>The LECO VX4 is a compact yet powerful inverted microscope designed for metallurgical and educational laboratories. It features a bright LED polarized light source suitable for both mounted and unmounted samples, delivering excellent contrast and image clarity. Engineered for strong optical performance and intuitive operation, the VX4 combines modern imaging technology with automated functionality to support demanding material investigations.</p><p>The VX4 is well suited for microstructural analysis such as <strong>grain size determination</strong>, <strong>pearlite/ferrite evaluation</strong>, <strong>nodularity assessment, dendrite arm spacing measurements</strong>, and <strong>advanced failure analysis</strong>. Full compatibility with LECO’s analytical software enhances efficiency in image capture, analysis, data management, and reporting, making the VX4 a practical and future-ready solution for metallography and materials characterization.</p><h4><strong>Key Features of the VX4</strong></h4><ul><li>Variable LED light source with built-in lever condenser, including field and aperture diaphragms</li><li>Trinocular viewing head with 10× / 22 mm adjustable focusing eyepieces</li><li>Revolving nosepiece accommodating up to five objectives</li><li>Standard objectives: 5×, 10×, 20×, and 50×</li><li>Optional 100× objective available</li><li>Brightfield observation with 360° polarizer/analyzer</li><li>Coaxial coarse and fine focus controls for precise adjustment</li><li>Ergonomic mechanical XY stage for smooth sample positioning</li></ul>

Thermo Scientific DXR3xi Raman Imaging Microscope

High-performance Raman imaging microscope offering fast, non-destructive 2D and 3D chemical imaging with intuitive workflows, automated calibration, and advanced data visualization.

<p><strong>The Thermo Scientific™ DXR3xi Raman Imaging Microscope delivers research-grade Raman imaging faster than ever before. Enhanced software features combined with higher spatial resolution allow users to instantly obtain detailed visual and chemical information. Advanced imaging capabilities, minimal sample preparation, and intuitive software provide researchers with the power of Raman spectroscopy at the speed modern research demands.</strong></p><h3><strong>Key features and benefits</strong></h3><ul><li><strong>Simple operation</strong> suitable for users of all skill levels</li><li><strong>Faster data visualization</strong> enabled by advanced imaging software<ul><li>Advanced particle analysis for rapid identification and analysis of microscopic contaminants</li><li>3D confocal imaging for non-destructive, non-invasive three-dimensional chemical and molecular investigations</li><li>Terrain Mapping to characterize uneven sample surfaces and easily acquire in-focus Raman images</li></ul></li><li><strong>Intuitive workflow</strong> designed for demanding applications to maximize sample throughput</li><li><strong>Automated calibration</strong> to improve efficiency</li><li><strong>High measurement accuracy</strong> supported by:<ul><li>Automatic alignment and calibration with no tools required</li><li>Automatic background compensation</li></ul></li><li><strong>Rapid system reconfiguration</strong> within seconds – pre-aligned lasers, filters, and gratings can be changed without tools</li><li><strong>Fast spectral analysis and interpretation</strong> using powerful <strong>Thermo Scientific™ OMNIC™xi Software</strong></li><li><strong>Advanced autofocus and morphological analysis</strong> to track positions across uneven surfaces</li><li><strong>Visualization tools</strong> for extracting chemical contrast and identifying and ranking features of interest</li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_8_9021ee32c0.jpg" alt="Thermo Scientific DXR3xi Raman Imaging Microscope " srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_8_9021ee32c0.jpg 234w," sizes="100vw" width="650" height="433"></p><h3><strong>Laser safety</strong></h3><ul><li>Microscope designed and independently certified as <strong>Class 1 laser safe</strong></li><li>Optional fiber optic accessories and selected components are <strong>Class 3b laser devices</strong>, requiring appropriate laser safety measures and protective eyewear</li><li>Laser path is physically blocked from the visual viewing path to prevent eye exposure during observation</li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_4_73e61c6ef9.jpg" alt="Thermo Scientific DXR3xi Raman Imaging Microscope " srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_4_73e61c6ef9.jpg 236w," sizes="100vw" width="650" height="430"></p><h3><strong>Applications</strong></h3><ul><li>Nanotechnology</li><li>Microplastics analysis</li><li>Polymer and chemical analysis</li><li>Electronics</li><li>Materials science</li><li>Academic research</li><li>Pharmaceutical research</li><li>Geology</li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_9_5d3708416c.jpg" alt="Thermo Scientific DXR3xi Raman Imaging Microscope " srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_9_5d3708416c.jpg 156w," sizes="100vw" width="650" height="650"></p><h3><strong>Specifications</strong></h3><ul><li><strong>Electrical Requirements</strong>: 100/240 V, 47/63 Hz</li><li><strong>Electronic Records and Signatures</strong>: 21CFR Part 11</li><li><strong>For Use With (Application)</strong>: Nanotechnology, Material science, Academic research, Pharmaceutical, Geology, Microplastics, Polymer/Chemical and Electronics</li><li><strong>Laser Power</strong>: Fine Laser Power Control: Power controlled and reported at samples in 0.1 mW increments</li><li><strong>Model</strong>: DXR3xi Raman Imaging Microscope</li><li><strong>Operating Temperature Range</strong>: 16°C to 27°C</li><li><strong>Resolution</strong>: Spatial: 0.5 µm; Confocal Depth: 2 µm</li><li><strong>Software Details</strong>: Data analysis and spectral interpretation with powerful Thermo Scientific™ OMNIC™xi Software</li><li><strong>Wavelength Range</strong>: 455 nm; 532 nm high brightness; 532 nm high power; 633 nm high brightness; 633 nm high power; 780 nm</li><li><strong>Type</strong>: Raman Imaging Microscope</li><li><strong>Unit Size</strong>: Each</li></ul>

Thermo Scientific DXR3 Raman Microscope

The Thermo Scientific DXR3 Raman Microscope is an easy-to-use confocal Raman system with automated calibration, high stability, and flexible laser options for a wide range of applications.

<p><strong>The </strong><span><strong>Thermo Scientific</strong></span><strong>™ DXR3 Raman Microscope is a modern, easy-to-use point-and-shoot Raman microscope designed to provide faster, more reliable access to Raman data than ever before. Advanced imaging capabilities combined with automated system calibration deliver exceptional stability, reproducibility, and confidence in Raman measurements—even for non-specialist users.</strong></p><p>Thanks to Automated X-axis Calibration, the DXR3 system maintains long-term accuracy and reliability while minimizing user intervention. With a flexible choice of lasers and gratings, the DXR3 Raman Microscope is ideally suited for applications across pharmaceutical research, academia, advanced polymers, microplastics, and many other demanding fields.</p><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3_Raman_Microscope_6_1dd5de4a21.jpg" alt="Thermo Scientific DXR3 Raman Microscope" srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3_Raman_Microscope_6_1dd5de4a21.jpg 245w," sizes="100vw" width="650" height="299"></p><h3><strong>Key capabilities</strong></h3><ul><li>New <strong>Particle Analysis</strong> functionality for rapid identification and analysis of microparticles</li><li>High-performance <strong>confocal Raman microscopy</strong> in a robust, fully integrated design</li><li>Fully automated <strong>alignment and calibration</strong> with no tools or manual procedures required</li><li>Real-time preview, automated fluorescence correction, auto-exposure, and cosmic ray rejection</li><li>System status indicator providing at-a-glance confirmation that the instrument is optimized and ready for data acquisition</li><li>Three-path fine-beam autoalignment to maintain peak performance and sampling integrity</li><li>Active laser power regulation ensuring consistent sample excitation throughout the lifetime of the laser</li><li>Advanced spectrograph design with no moving parts for simplified operation and highly robust detection and calibration</li><li>Pre-aligned, lock-in-place components with automatic recognition and stored alignment, enabling system reconfiguration in seconds</li><li>Interchangeable lasers and components shared across the DXR3 Raman family</li><li>Optional automated <strong>polarized Raman spectroscopy</strong> for structural information complementary to chemical data</li><li>Add new excitation wavelengths without tools or service engineer intervention</li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3_Raman_Microscope_2_e366caa151.jpg" alt="Thermo Scientific DXR3 Raman Microscope" srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3_Raman_Microscope_2_e366caa151.jpg 204w," sizes="100vw" width="631" height="483"></p><h3><strong>Laser safety</strong></h3><ul><li>Microscope independently certified as <strong>Class 1 laser safe</strong><br><i>(Note: optional fiber-optic accessories and certain other optional components are Class 3B laser devices and require appropriate laser safety precautions and eyewear)</i></li><li>Laser is physically blocked from the visual viewing path, preventing eye exposure during sample observation</li></ul><h3><strong>Validation and compliance</strong></h3><ul><li>Complete <strong>DQ/IQ/OQ/PQ validation</strong> package available, including extensive documentation and automated software protocols</li><li><strong>OMNIC™ D/S software</strong> supports compliance with <strong>21 CFR Part 11</strong></li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3_Raman_Microscope_3_62f6baad12.jpg" alt="Thermo Scientific DXR3 Raman Microscope" srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3_Raman_Microscope_3_62f6baad12.jpg 178w," sizes="100vw" width="630" height="553"></p><h3><strong>Exceptional analytical performance</strong></h3><ul><li>Spatial resolution down to <strong>540 nm</strong> on ideal samples</li><li>Confocal depth resolution as fine as <strong>1.7 µm</strong> on ideal samples</li><li>Full spectral range of <strong>3500–50 cm⁻¹</strong> captured in a single CCD exposure, eliminating stitching artifacts</li><li>Extended spectral range up to <strong>6000 cm⁻¹</strong> available with the 532 nm laser</li><li>Support for multiple excitation lasers: <strong>455, 532, 633, and 785 nm</strong> (high-brightness and high-power options)</li><li>Automatic fluorescence correction available for all excitation lasers</li><li>Research-grade <strong>Olympus</strong> viewing optics</li><li>Automatic intensity correction enabling spectral comparability between instruments and across different excitation lasers</li><li>Multidimensional wavelength calibration ensuring accurate calibration across the entire spectral range</li><li>Proprietary <strong>Triplet spectrograph</strong> delivering exceptional peak shape and maintaining focus at all wavelengths</li><li>Software-controlled switching between confocal and high-energy collection modes</li><li>Proprietary algorithms for automated cosmic ray rejection and high-quality laser line filters for artifact-free spectra</li><li>Depolarized lasers to eliminate confusing sample orientation effects</li><li>Active laser power monitoring ensures reproducible excitation power over the laser lifetime and after laser replacement</li><li>Optimized gratings for each excitation laser, avoiding performance compromises associated with shared gratings</li><li>Proprietary autoalignment maintains the system in like-new condition</li><li>Smart-Backgrounds technology automatically removes the CCD dark energy profile</li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3_Raman_Microscope_5_ca01560747.jpg" alt="Thermo Scientific DXR3 Raman Microscope" srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3_Raman_Microscope_5_ca01560747.jpg 210w," sizes="100vw" width="633" height="471"></p><h3><strong>Recommended applications</strong></h3><ul><li><strong>Forensics</strong> – trace evidence analysis and illicit drug identification</li><li><strong>Pharmaceuticals</strong> – polymorphism studies, particulate contamination, and diffusion analysis</li><li><strong>Art restoration and conservation</strong> – identification and characterization of pigments, resins, glazes, and inks</li><li><strong>Archaeology</strong> – characterization of horn, shell, bone, and ceramic artifacts</li><li><strong>Solar materials</strong> – silicon crystallinity and photovoltaic material characterization</li><li><strong>Polymers</strong> – inclusions, gel defects, weathering effects, laminate layers, and crystallinity</li><li><strong>Failure analysis</strong> – characterization of particulates and small surface features</li><li><strong>Gemology</strong> – rapid identification of colored stones, differentiation of natural and synthetic diamonds, characterization of inclusions and adulterants</li><li><strong>Nanotechnology</strong> – graphene, carbon nanotubes (CNTs), DLC coatings, and other nanostructures</li><li><strong>Academic research</strong> – materials science, biological studies, and a wide range of applied research fields</li></ul><p><img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_9_5d3708416c.jpg" alt="Thermo Scientific DXR3 Raman Microscope" srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_Thermo_Scientific_DXR_3xi_Raman_Imaging_Microscope_9_5d3708416c.jpg 156w," sizes="100vw" width="650" height="650"></p><h3><strong>Specification</strong></h3><ul><li><strong>Depth (Metric):</strong> 68 cm</li><li><strong>Description:</strong> DXR3 Raman Microscope</li><li><strong>Electrical Requirements:</strong> 100/240 V, 47/63 Hz</li><li><strong>Electronic Records and Signatures:</strong> 21CFR Part 11</li><li><strong>For Use With (Application):</strong>&nbsp;<ul><li>Pharmaceutical</li><li>Microplastics</li><li>Forensics</li><li>Polymer/Chemical</li><li>Petrochemical</li><li>Material Science</li><li>Nanomaterials</li><li>Academia</li><li>Energy Storage</li><li>Art Restoration/Conservation</li></ul></li><li><strong>Height (Metric):</strong> 61 cm</li><li><strong>Laser Power:</strong> Fine Laser Power Control: Power controlled and reported at samples in 0.1 mW increments</li><li><strong>Model:</strong> DXR3</li><li><strong>Operating Temperature Range:</strong> 16°C to 27 °C</li><li><strong>Resolution:</strong>&nbsp;<ul><li><strong>Spatial:</strong> 1 µm</li><li><strong>Confocal Depth:</strong> 2 µm</li></ul></li><li><strong>Wavelength Range:</strong>&nbsp;<ul><li>455 nm</li><li>532 nm high brightness</li><li>532 nm high power</li><li>633 nm high brightness</li><li>633 nm high power</li><li>780 nm</li></ul></li><li><strong>Weight (Metric):</strong> 66.5 kg</li><li><strong>Width (Metric):</strong> 94 cm</li><li><strong>Type:</strong> Microscope</li><li><strong>Unit Size:</strong> Each</li></ul>

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